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1.
Using ESR and optical spectroscopy we showed that the blue coloring is imparted to natural apatites by SO 3 radicals and the green coloring is due to SiO 3 radicals complexed with rare earth ions, SiO 3 -(Ce3++K). The role of U4+ and Th4+ isomorphous actinide ions in the process of color center formation is investigated. United Institute of Geology, Geophysics, and Mineralogy, Siberian Branch, Russian Academy of Sciences. Translated fromZhurnal Struktumoi Khimii, Vol. 36, No. 1, pp. 89–101, January–February, 1995. Translated by L. Smolina  相似文献   

2.
Single crystals of U3+:LaBr3 were grown by the Bridgman-Stockbarger technique. High-resolution polarized absorption spectra of the crystals were recorded at 4.2 K in the 4000-50,000 cm−1 range. Sixty-four experimental crystal-field energy levels of the U3+ ion were fitted to a semiempirical Hamiltonian employing free-ion, one-electron crystal-field as well as two-particle correlation crystal-field (CCF) operators with an r.m.s. deviation of 28 cm−1. The performed analysis of the spectra enabled the determination of crystal-field parameters and assignment of the observed 5f3→5f3 transitions. The effects of selected CCF operators on the splitting of some specific U3+ multiplets have been investigated and the obtained values of Hamiltonian parameters are discussed and compared with those reported in previous analyses.  相似文献   

3.
Prof. Ran Friedman 《Chemphyschem》2023,24(2):e202200516
The use of actinides for medical, scientific and technological purposes has gained momentum in the recent years. This creates a need to understand their interactions with biomolecules, both at the interface and as they become complexed. Calculation of the Gibbs binding energies of the ions to biomolecules, i. e., the Gibbs energy change associated with a transfer of an ion from the water phase to its binding site, could help to understand the actinides’ toxicities and to design agents that bind them with high affinities. To this end, there is a need to obtain accurate reference values for actinide hydration, that for most actinides are not available from experiment. In this study, a set of ionic radii is developed that enables future calculations of binding energies for Pu3+ and five actinides with renewed scientific and technological interest: Ac3+, Am3+, Cm3+, Bk3+ and Cf3+. Reference hydration energies were calculated using quantum chemistry and ion solvation theory and agree well for all ions except Ac3+, where ion solvation theory seems to underestimate the magnitude of the Gibbs hydration energy. The set of radii and reference energies that are presented here provide means to calculate binding energies for actinides and biomolecules.  相似文献   

4.
Polycrystalline uranium-bearing compounds Y6U1O12, Gd6U1O12, Ho6U1O12, Yb6U1O12, and Lu6U1O12 samples were irradiated with various ions species (300 keV Kr++, 400 keV Ne++, and 100 keV He+) at cryogenic temperature (∼100 K), and the microstructures were examined following irradiation using grazing incidence X-ray diffraction and transmission electron microscopy. The pristine samples are characterized by an ordered, fluorite derivative structure, known as the delta phase. This structure possesses rhombohedral symmetry. Amorphization was not observed in any of the irradiated samples, even at the highest dose ∼65 dpa (displacement per atom). On the other hand, some of these compounds experienced an order-to-disorder (O-D) phase transformation, from an ordered rhombohedral to a disordered fluorite structure, at ion doses between 2.5 and 65 dpa, depending on ion irradiation species. Factors influencing the irradiation-induced O-D transformation tendencies of these compounds are discussed in terms of density functional theory calculations of the O-D transformation energies.  相似文献   

5.
An atomistic study is presented on the phase stability, site preference and lattice constants of the actinide intermetallic compounds Th3Co4+xAl12−x and U3Co4+xAl12−x. Calculations are based on a series of interatomic pair potentials related to the actinides and transition metals, which are obtained by a strict lattice inversion method. The lattice constants of Th3Co4+xAl12−x and U3Co4+xAl12−x are calculated for different values of x. The site preference of Co atoms at Al sites is also evaluated and the order is given as 6h, 4f, 2b and 12k for Th3Co4+xAl12−x, and 6h, 4f, 12k and 2b for U3Co4+xAl12−x. In addition, some simple mechanical properties such as the elastic constants and bulk modulus are investigated for the actinide compounds with complex structures.  相似文献   

6.
Garnet-structure related metal oxides with the nominal chemical composition of Li5La3Nb2O12, In-substituted Li5.5La3Nb1.75In0.25O12 and K-substituted Li5.5La2.75K0.25Nb2O12 were prepared by solid-state reactions at 900, 950, and 1000 °C using appropriate amounts of corresponding metal oxides, nitrates and carbonates. The powder XRD data reveal that the In- and K-doped compounds are isostructural with the parent compound Li5La3Nb2O12. The variation in the cubic lattice parameter was found to change with the size of the dopant ions, for example, substitution of larger In3+(rCN6: 0.79 Å) for smaller Nb5+ (rCN6: 0.64 Å) shows an increase in the lattice parameter from 12.8005(9) to 12.826(1) Å at 1000 °C. Samples prepared at higher temperatures (950, 1000 °C) show mainly bulk lithium ion conductivity in contrast to those synthesized at lower temperatures (900 °C). The activation energies for the ionic conductivities are comparable for all samples. Partial substitution of K+ for La3+ and In3+ for Nb5+ in Li5La3Nb2O12 exhibits slightly higher ionic conductivity than that of the parent compound over the investigated temperature regime 25-300 °C. Among the compounds investigated, the In-substituted Li5.5La3Nb1.75In0.25O12 exhibits the highest bulk lithium ion conductivity of 1.8×10−4 S/cm at 50 °C with an activation energy of 0.51 eV. The diffusivity (“component diffusion coefficient”) obtained from the AC conductivity and powder XRD data falls in the range 10−10-10−7 cm2/s over the temperature regime 50-200 °C, which is extraordinarily high and comparable with liquids. Substitution of Al, Co, and Ni for Nb in Li5La3Nb2O12 was found to be unsuccessful under the investigated conditions.  相似文献   

7.
The (13E,19E)-N1′,N3′-bis[4-(diethylamino)-2-hydroxybenzylidene]malonohydrazide (L) has been developed for the detection of Th4+ ions using dual channel signalling system. The UV–vis absorbance and fluorescence spectroscopic data revealed the formation of L–Th4+ complex in 1:1 equilibrium. The density functional theory (DFT) also confirms the optimum binding cavity for the recognition of metal ion. The binding constant computed from different mathematical models for an assembly of L–Th4+. The detection limit of L for Th4+ recognition is to a concentration down to 0.1 μM (0.023 μg g−1). The present sensing system is also successfully applied for the detection of Th4+ ion present in soil near nuclear atomic plants.  相似文献   

8.
The ordered double perovskites ALaMgTaO6 (A=Ba, Sr, Ca) and La2Mg(Mg1/3Ta2/3)O6 have been prepared and characterized. Synchrotron X-ray powder diffraction analyses show that all four compounds exhibit a rock-salt type ordering of the B-site cations (Mg2+/Ta5+) and a random distribution of A-site cations (A2+/La3+). The space group symmetries are determined to be for BaLaMgTaO6, and P21/n for SrLaMgTaO6, CaLaMgTaO6, and La2Mg(Mg1/3Ta2/3)O6. Diffuse-reflectance spectroscopy shows these ordered perovskites have optical band gaps in the range of 4.6−4.8 eV. These values are roughly 1 eV wider than the ternary perovskite oxides of Ta5+ such as KTaO3, due to narrowing of the conduction bandwidth which results from Mg2+/Ta5+ ordering. These compounds are insulators with dielectric permittivities of κ=18-23, dielectric losses of tan δ=0.004-0.007, and small temperature coefficients of capacitance <100 ppm/K over the temperature range 20-150 °C. BaLaMgTaO6 is of particular interest because it possesses a near-zero temperature dependence of capacitance.  相似文献   

9.
The geometry of metal ions (La3+, Ce3+, UO, and Th4+) complexes with 5‐azorhodanine derivatives was optimized at the level of molecular mechanics. Two stoichiometric ratios of metal to ligand (i.e., 1:1 and 1:2) were investigated. Tetracoordinate and hexacoordinate of each stoichiometric ratio have been studied. Effect of substitution in the ligand on the geometry of the complexes was discussed in the light of electron donating–accepting properties of these substituents. The influence of the nuclear effective charge of the central metal ions on the metal–ligand (M–L) bonding was discussed and the effect of the number of ligands on the M–L bond length was also discussed and correlated to the experimental results. The total energies of the different metal complexes were computed using the extended Huckel method. The effect of substituents in ligand, metal type, and stoichiometry of the complexes on the complex total energies were discussed. Stability constant of (La3+, Ce3+, UO, and Th4+) metal ions with 5‐azorhodanine derivaties have been determined potentiometrically in 0.1 M KCl and 50% (v/v) ethanol–water mixture. The order of the stability constants of the formed complexes was found to be La3+ < Ce3+ < UO < Th4+. The influence of substituents on the stability of the complexes was examined on the basis of electron‐repelling property of the substituent. The effect of temperature on the stability of the complexes formed was studied and the corresponding thermodynamic parameters (ΔG, ΔH, and ΔS) were derived and discussed. The stoichiometries of these complexes were determined conductometrically and indicated the formation of 1:1 and 1:2 (metal:ligand) complexes. © 2003 Wiley Periodicals, Inc. Int J Quantum Chem, 2003  相似文献   

10.
The possibility that the relative reactivity of complexes of actinide metals in the +2 and +3 oxidation states could be investigated by examining reactions between AnIII and AnII species of Th and U with rare-earth metal reagents that provide EPR confirmation of electron transfer reactivity has been explored. Neither Cp’’3ThIII nor Cp’’3UIII will reduce Cp’’3LaIII or Cp’3YIII (Cp’=C5H4SiMe3, Cp’’=C5H3(SiMe3)2). However, both [K(2.2.2-cryptand)][Cp’’3ThII] and [K(2.2.2-cryptand)][Cp’’3UII] reduce Cp’’3LaIII and Cp’3YIII to form [Cp’’3LaII]1− and [Cp’3YII]1−, respectively, which were identified by EPR spectroscopy. The reverse reactions also occur which indicates that the reduction potentials are similar. [Cp’’3LaII]1− reduces Cp’3YIII and the reverse YII/LaIII combination also occurs. In both cases, the reactions generate EPR spectra indicative of multiple species in the mixtures of LaII and YII, which is consistent with ligand exchange and demonstrates that numerous heteroleptic complexes of these LnII ions exist.  相似文献   

11.
Er3+ doped aluminophosphate glasses with various Na2O/Li2O ratios were prepared at 1250 °C using a silica crucible to study mixed alkali effect (MAE). The effect of relative alkali content on glass transition temperature, crystallization temperature and thermal stability were investigated using differential scanning calorimetry (DSC). In addition, apparent activation energies for crystallization, Ec, were determined employing the Kissinger equation. The effect of Al2O3 content on the magnitude of MAE was also discussed. No mixed-alkali effect is observed on crystallization temperature.  相似文献   

12.
The crystal and electronic structures, and luminescence properties of Eu2+, Ce3+ and Tb3+ activated LiSi2N3 are reported. LiSi2N3 is an insulator with an indirect band gap of about 5.0 eV (experimental value ∼6.4 eV) and the Li 2s, 2p states are positioned on the top of the valence band close to the Fermi level and the bottom of the conduction band. The solubility of Eu2+ is significantly higher than Ce3+ and Tb3+ in LiSi2N3 which may be strongly related to the valence difference between Li+ and rare-earth ions. LiSi2N3:Eu2+ shows yellow emission at about 580 nm due to the 4f65d1→4f7 transition of Eu2+. Double substitution is found to be the effective ways to improve the luminescence efficiency of LiSi2N3:Eu2+, especially for the partial replacement of (LiSi)5+ with (CaAl)5+, which gives red emission at 620 nm, showing highly promising applications in white LEDs. LiSi2N3:Ce3+ emits blue light at about 450 nm arising from the 5d1→4f15d0 transition of Ce3+ upon excitation at 320 nm. LiSi2N3:Tb3+ gives strong green line emission with a maximum peak at about 542 nm attributed to the 5D47FJ (J=3-6) transition of Tb3+, which is caused by highly efficient energy transfer from the LiSi2N3 host to the Tb3+ ions.  相似文献   

13.
Indion FR 10 is a commercially available ion exchange resin with sulphonic acid functionality named as H+ form, has appreciable defluoridation capacity (DC). It has been chemically modified to La3+, Fe3+, Ce3+ and Zr4+ forms by incorporating respective metal ions into the resin in order to know their fluoride selectivity by measuring the DC of the respective resin. The maximum DC of these chemically modified ion exchange resins namely La3+, Fe3+, Ce3+ and Zr4+ forms were found to be 469.7, 467.5, 456.3 and 470.9 mg F/kg respectively suggests their higher selectivity towards fluoride than H+ form which has the DC of only 275 mg F/kg at 11 mg/L initial fluoride concentration. The higher DC of the modified resins was explained by electrostatic adsorption and complexation whereas H+ form retains fluoride by hydrogen bond. The functional groups present in the sorbents were identified by FTIR and the existence of fluoride onto the resins was confirmed by EDAX analysis. The experimental data was fitted with both Freundlich and Langmuir isotherms. Thermodynamic parameters such as ΔG°, ΔH° and ΔS° indicate that the nature of sorption is spontaneous and endothermic. The applicability of reaction-based and diffusion-based kinetic models was investigated. A field trial was carried out with fluoride water collected from a nearby fluoride-endemic village to test the suitability of these sorbents at field conditions.  相似文献   

14.
The new quaternary sulfide La4MnCu6S10 has been synthesized by the reaction of La2S3, MnS, and CuS2 at 1223 K. This compound crystallizes in a new structure type in space group of the triclinic system with one formula unit in a cell of dimensions at 153 K of a=6.6076(3) Å, b=7.3247(3) Å, c=8.7844(4) Å, α=83.457(1)°, β=74.398(1)°, γ=89.996(1)°, and V=406.61(3) Å3. The structure of La4MnCu6S10 consists of a three-dimensional framework of interconnected LaS7 monocapped trigonal prisms, MnS6 octahedra, and CuS4 tetrahedra. Band gaps of 2.49 eV in the [100] direction and 2.53 eV in the [001] direction have been derived from optical absorption measurements on a La4MnCu6S10 single crystal.  相似文献   

15.
Thin crystals of La2O3, LaAlO3, La2/3TiO3, La2TiO5, and La2Ti2O7 have been irradiated in situ using 1 MeV Kr2+ ions at the Intermediate Voltage Electron Microscope-Tandem User Facility (IVEM-Tandem), Argonne National Laboratory (ANL). We observed that La2O3 remained crystalline to a fluence greater than 3.1×1016 ions cm−2 at a temperature of 50 K. The four binary oxide compounds in the two systems were observed through the crystalline-amorphous transition as a function of ion fluence and temperature. Results from the ion irradiations give critical temperatures for amorphisation (Tc) of 647 K for LaAlO3, 840 K for La2Ti2O7, 865 K for La2/3TiO3, and 1027 K for La2TiO5. The Tc values observed in this study, together with previous data for Al2O3 and TiO2, are discussed with reference to the melting points for the La2O3-Al2O3 and La2O3-TiO2 systems and the different local environments within the four crystal structures. Results suggest that there is an observable inverse correlation between Tc and melting temperature (Tm) in the two systems. More complex relationships exist between Tc and crystal structure, with the stoichiometric perovskite LaAlO3 being the most resistant to amorphisation.  相似文献   

16.
A new microflow injection chemiluminescence (μFI-CL) system was described for the determination of cisplatin in human serum. By using the microchip with double spiral channel configuration, the sensitivity was greatly enhanced due to more efficient mixing of the analyte and reagent solutions. Experimental results revealed that common ions in human serum, such as Mn2+, Co2+, Fe3+, Cu2+, Zn2+, Ni2+, Na+, K+, Ca2+, Cl, NO3, Ac, CO32−, PO43−, SO42− did not cause interference with the detection of Pt(II) by using 1,10-phenanthroline as the masking agent. Under the optimized conditions, a linear calibration curve (R2 = 0.998) over the range 2.0 × 10−8 to 2.0 × 10−6 mol L−1 was obtained with the detection limit of 1.24 × 10−9 mol L−1. The relative standard deviation was found to be 3.46% (n = 12) for 2.0 × 10−7 mol L−1. The sample consumption was only 2 μL with the sample throughput of 72 h−1. It had been used for trace platinum determination in cisplatin injection and human serum samples after the dosage of cisplatin. The recovery varied from 97.6 to 103.9%. The results proved that the proposed μFI-CL system had the advantages of high sensitivity and precision, low sample and reagents consumption, and high analytical throughput.  相似文献   

17.
The total conductivity of monoclinic La2Ti2SiO9 is mixed oxygen-ionic and n-type electronic, and increases on reduction of the oxygen partial pressure down to 10−21 atm at 973-1223 K. The substitution of Ti4+ with Nb5+ decreases both contributions to the conductivity, whilst Pr doping and reducing p(O2) have opposite effects. The oxygen ion transference numbers of La2Ti2SiO9−δ, LaPrTi2SiOδ and La2Ti1.8Nb0.2SiOδ ceramics, measured by the faradaic efficiency and e.m.f. methods, vary in the range 0.15-0.32, increasing when temperature decreases. In air, the activation energies for the ionic and electronic transport are 1.23-1.40 and 1.59-1.74 eV, respectively. Protonic contribution to the conductivity in wet atmospheres becomes significant at temperatures below 1000 K. The experimental data and the results of atomistic computer simulations suggest that the oxygen-ionic and electronic transport is primarily determined by processes involving TiO6 octahedra. The ionic conduction may occur via both the vacancy and interstitial migration mechanisms, but the former is more favorable energetically and should dominate, at least, in reducing atmospheres. The average thermal expansion coefficients of La2Ti2SiO9-based ceramics, calculated from dilatometric data in air, are (8.7−9.5)×10−6 K−1 at 300-1373 K. The lattice of lanthanum titanate-silicate is almost intolerant with respect to A-site deficiency and to doping with lower-valence cations, such as Sr and Fe.  相似文献   

18.
A new ternary compound, U3Co2Ge7, has been synthesized from the corresponding elements by a high temperature reaction using molten tin flux. It crystallizes in the orthorhombic La3Co2Sn7-type (Pearson's symbol oC24, space group Cmmm, No. 65) with lattice parameters determined from single-crystal X-ray diffraction as follows: a=4.145(2) Å; b=24.920(7); c=4.136(2) Å, V=427.2(3) Å3. Structure refinements confirm an ordered structure having two crystallographically inequivalent uranium atoms, occupying sites with dissimilar coordination. U3Co2Ge7 orders ferromagnetically below 40 K and undergoes a consecutive magnetic transition at 20 K. These results have been obtained from temperature- and field-dependent magnetization, resistivity and heat-capacity measurements. The estimated Sommerfeld coefficient γ=87 mJ/mol-U K2 suggests U3Co2Ge7 to be a moderately heavy-fermion material.  相似文献   

19.
The unusual oxidation state +3 of the thorium has been stabilized into a lithium containing non-stoichiometric mixed-valence (III/IV) thorium fluorinated phase with formula Li2+xTh12F50 (0<x<1.8). This phase is closely related to the Li5.5Ce12F50 one, the structure of which has been determined from the combined single-crystal X-ray diffraction and high resolution synchrotron powder diffraction. In these phases, the Li+ ions can be divided into two groups and are located either in locked positions or in open channels of the three dimensional framework. The amount of Li+ ions in open channels can be variable, so that the afore mentioned single phase may be considered as an insertion compound. The Li+ insertion is accompanied by the simultaneous reduction of a part of the Th4+ ions, resulting in a mixed-valence III/IV thorium fluoride. The electrochemical insertion of Li+ ions into the open channels of the host matrix has been carried out at 60 °C, using an alkylcarbonate PC-LiClO4 1 M electrolyte. The Li+ and Th3+ contents, both in the starting composition and the Li+ inserted ones, were investigated by high resolution solid state 7Li NMR and EPR, respectively.  相似文献   

20.
In this study, a new poly(vinyl chloride) (PVC) membrane sensor for La3+ ion based on 2,2′-dithiodipyridine as an ion carrier was prepared. This electrode revealed good selectivity for La3+ over a wide variety of other metal ions. Effects of experimental parameters such as membrane composition, nature and amount of plasticizer, the amount of additive and concentration of internal solution on the potential response of La3+ sensor were investigated. The electrode exhibited a Nernstian slope of 20.0 ± 1.0 mV per decade of La3+ over a concentration range of 7.1 × 10−6 to 2.2 × 10−2 M of La3+ in the pH range 3.3-8.0. The response time was about 7 s and the detection limit was 3.1 × 10−6 M. The electrode can be used for at least 2 months without a considerable divergence in potential. The proposed electrode was used as an indicator electrode in potentiometric titration of oxalate and fluoride ions and was applied for determination of F ion in mouthwash solution.  相似文献   

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